{"bundle_type":"pith_open_graph_bundle","bundle_version":"1.0","pith_number":"pith:2017:T3V4A52P46KR7SEPQHK3LMLTQO","short_pith_number":"pith:T3V4A52P","canonical_record":{"source":{"id":"1705.03293","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-05-09T12:35:46Z","cross_cats_sorted":["cond-mat.quant-gas","physics.atom-ph"],"title_canon_sha256":"fff0d5bc5e233b186ca77360e8fc6c1d673d740900c074061a01978882de99bc","abstract_canon_sha256":"e524ce4d206fe76a773ade625406637962ab05a87440921468e336157f173cc4"},"schema_version":"1.0"},"canonical_sha256":"9eebc0774fe7951fc88f81d5b5b173839f8465e52cb06cd9a59f4796bb08b6ab","source":{"kind":"arxiv","id":"1705.03293","version":1},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1705.03293","created_at":"2026-05-18T00:38:41Z"},{"alias_kind":"arxiv_version","alias_value":"1705.03293v1","created_at":"2026-05-18T00:38:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1705.03293","created_at":"2026-05-18T00:38:41Z"},{"alias_kind":"pith_short_12","alias_value":"T3V4A52P46KR","created_at":"2026-05-18T12:31:43Z"},{"alias_kind":"pith_short_16","alias_value":"T3V4A52P46KR7SEP","created_at":"2026-05-18T12:31:43Z"},{"alias_kind":"pith_short_8","alias_value":"T3V4A52P","created_at":"2026-05-18T12:31:43Z"}],"events":[{"event_type":"record_created","subject_pith_number":"pith:2017:T3V4A52P46KR7SEPQHK3LMLTQO","target":"record","payload":{"canonical_record":{"source":{"id":"1705.03293","kind":"arxiv","version":1},"metadata":{"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-05-09T12:35:46Z","cross_cats_sorted":["cond-mat.quant-gas","physics.atom-ph"],"title_canon_sha256":"fff0d5bc5e233b186ca77360e8fc6c1d673d740900c074061a01978882de99bc","abstract_canon_sha256":"e524ce4d206fe76a773ade625406637962ab05a87440921468e336157f173cc4"},"schema_version":"1.0"},"canonical_sha256":"9eebc0774fe7951fc88f81d5b5b173839f8465e52cb06cd9a59f4796bb08b6ab","receipt":{"kind":"pith_receipt","key_id":"pith-v1-2026-05","algorithm":"ed25519","signed_at":"2026-05-18T00:38:41.590272Z","signature_b64":"C3Hmybogu0YUkRTqha4G0l0QUSN8ZMHBWbpQrT1j3v8/JBq8m+O/joskmvN2IeowtNiErITyyBCv9upqM0VlBw==","signed_message":"canonical_sha256_bytes","builder_version":"pith-number-builder-2026-05-17-v1","receipt_version":"0.3","canonical_sha256":"9eebc0774fe7951fc88f81d5b5b173839f8465e52cb06cd9a59f4796bb08b6ab","last_reissued_at":"2026-05-18T00:38:41.589762Z","signature_status":"signed_v1","first_computed_at":"2026-05-18T00:38:41.589762Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"source_kind":"arxiv","source_id":"1705.03293","source_version":1,"attestation_state":"computed"},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:38:41Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"9u1xlbTF3U58swvHIbU+qcERFWiZzsZLBOhGd0c5dXmWdWknYVzpoqR9TwOYlgn+NgVz2/F//w1urDSlI2stDA==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T18:53:58.605591Z"},"content_sha256":"5959ed205d0805d4fff84fb6b07dabeacef6658613a7491e36ba222dc245f46f","schema_version":"1.0","event_id":"sha256:5959ed205d0805d4fff84fb6b07dabeacef6658613a7491e36ba222dc245f46f"},{"event_type":"graph_snapshot","subject_pith_number":"pith:2017:T3V4A52P46KR7SEPQHK3LMLTQO","target":"graph","payload":{"graph_snapshot":{"paper":{"title":"Local optical control of the resonant dipole-dipole interaction between Rydberg atoms","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","headline":"","cross_cats":["cond-mat.quant-gas","physics.atom-ph"],"primary_cat":"quant-ph","authors_text":"Antoine Browaeys, Daniel Barredo, Sylvain de L\\'es\\'eleuc, Thierry Lahaye, Vincent Lienhard","submitted_at":"2017-05-09T12:35:46Z","abstract_excerpt":"We report on the local control of the transition frequency of a spin-$1/2$ encoded in two Rydberg levels of an individual atom by applying a state-selective light shift using an addressing beam. With this tool, we first study the spectrum of an elementary system of two spins, tuning it from a non-resonant to a resonant regime, where \"bright\" (superradiant) and \"dark\" (subradiant) states emerge. We observe the collective enhancement of the microwave coupling to the bright state. We then show that after preparing an initial single spin excitation and letting it hop due to the spin-exchange inter"},"claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1705.03293","kind":"arxiv","version":1},"verdict":{"id":null,"model_set":{},"created_at":null,"strongest_claim":"","one_line_summary":"","pipeline_version":null,"weakest_assumption":"","pith_extraction_headline":""},"references":{"count":0,"sample":[],"resolved_work":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","internal_anchors":0},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"author_claims":{"count":0,"strong_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"builder_version":"pith-number-builder-2026-05-17-v1"},"verdict_id":null},"signer":{"signer_id":"pith.science","signer_type":"pith_registry","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54"},"created_at":"2026-05-18T00:38:41Z","supersedes":[],"prev_event":null,"signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"pNaMA/1QyqAUKhnGTFf7iTJBC3y9nYmkZ1F9tyl+Z1XU8tmIaioirGLz2rhKXNZP0uoqpu4ozpFDV/0SNOVaBg==","signed_message":"open_graph_event_sha256_bytes","signed_at":"2026-05-30T18:53:58.605995Z"},"content_sha256":"fe3b8130104326d282d91d304e1a20caf6dbb5805ced8ad65b7f2bc397b767e3","schema_version":"1.0","event_id":"sha256:fe3b8130104326d282d91d304e1a20caf6dbb5805ced8ad65b7f2bc397b767e3"}],"timestamp_proofs":[],"mirror_hints":[{"mirror_type":"https","name":"Pith Resolver","base_url":"https://pith.science","bundle_url":"https://pith.science/pith/T3V4A52P46KR7SEPQHK3LMLTQO/bundle.json","state_url":"https://pith.science/pith/T3V4A52P46KR7SEPQHK3LMLTQO/state.json","well_known_bundle_url":"https://pith.science/.well-known/pith/T3V4A52P46KR7SEPQHK3LMLTQO/bundle.json","status":"primary"}],"public_keys":[{"key_id":"pith-v1-2026-05","algorithm":"ed25519","format":"raw","public_key_b64":"stVStoiQhXFxp4s2pdzPNoqVNBMojDU/fJ2db5S3CbM=","public_key_hex":"b2d552b68890857171a78b36a5dccf368a953413288c353f7c9d9d6f94b709b3","fingerprint_sha256_b32_first128bits":"RVFV5Z2OI2J3ZUO7ERDEBCYNKS","fingerprint_sha256_hex":"8d4b5ee74e4693bcd1df2446408b0d54","rotates_at":null,"url":"https://pith.science/pith-signing-key.json","notes":"Pith uses this Ed25519 key to sign canonical record SHA-256 digests. Verify with: ed25519_verify(public_key, message=canonical_sha256_bytes, signature=base64decode(signature_b64))."}],"merge_version":"pith-open-graph-merge-v1","built_at":"2026-05-30T18:53:58Z","links":{"resolver":"https://pith.science/pith/T3V4A52P46KR7SEPQHK3LMLTQO","bundle":"https://pith.science/pith/T3V4A52P46KR7SEPQHK3LMLTQO/bundle.json","state":"https://pith.science/pith/T3V4A52P46KR7SEPQHK3LMLTQO/state.json","well_known_bundle":"https://pith.science/.well-known/pith/T3V4A52P46KR7SEPQHK3LMLTQO/bundle.json"},"state":{"state_type":"pith_open_graph_state","state_version":"1.0","pith_number":"pith:2017:T3V4A52P46KR7SEPQHK3LMLTQO","merge_version":"pith-open-graph-merge-v1","event_count":2,"valid_event_count":2,"invalid_event_count":0,"equivocation_count":0,"current":{"canonical_record":{"metadata":{"abstract_canon_sha256":"e524ce4d206fe76a773ade625406637962ab05a87440921468e336157f173cc4","cross_cats_sorted":["cond-mat.quant-gas","physics.atom-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-05-09T12:35:46Z","title_canon_sha256":"fff0d5bc5e233b186ca77360e8fc6c1d673d740900c074061a01978882de99bc"},"schema_version":"1.0","source":{"id":"1705.03293","kind":"arxiv","version":1}},"source_aliases":[{"alias_kind":"arxiv","alias_value":"1705.03293","created_at":"2026-05-18T00:38:41Z"},{"alias_kind":"arxiv_version","alias_value":"1705.03293v1","created_at":"2026-05-18T00:38:41Z"},{"alias_kind":"doi","alias_value":"10.48550/arxiv.1705.03293","created_at":"2026-05-18T00:38:41Z"},{"alias_kind":"pith_short_12","alias_value":"T3V4A52P46KR","created_at":"2026-05-18T12:31:43Z"},{"alias_kind":"pith_short_16","alias_value":"T3V4A52P46KR7SEP","created_at":"2026-05-18T12:31:43Z"},{"alias_kind":"pith_short_8","alias_value":"T3V4A52P","created_at":"2026-05-18T12:31:43Z"}],"graph_snapshots":[{"event_id":"sha256:fe3b8130104326d282d91d304e1a20caf6dbb5805ced8ad65b7f2bc397b767e3","target":"graph","created_at":"2026-05-18T00:38:41Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"graph_snapshot":{"author_claims":{"count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57","strong_count":0},"builder_version":"pith-number-builder-2026-05-17-v1","claims":{"count":0,"items":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"formal_canon":{"evidence_count":0,"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"paper":{"abstract_excerpt":"We report on the local control of the transition frequency of a spin-$1/2$ encoded in two Rydberg levels of an individual atom by applying a state-selective light shift using an addressing beam. With this tool, we first study the spectrum of an elementary system of two spins, tuning it from a non-resonant to a resonant regime, where \"bright\" (superradiant) and \"dark\" (subradiant) states emerge. We observe the collective enhancement of the microwave coupling to the bright state. We then show that after preparing an initial single spin excitation and letting it hop due to the spin-exchange inter","authors_text":"Antoine Browaeys, Daniel Barredo, Sylvain de L\\'es\\'eleuc, Thierry Lahaye, Vincent Lienhard","cross_cats":["cond-mat.quant-gas","physics.atom-ph"],"headline":"","license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-05-09T12:35:46Z","title":"Local optical control of the resonant dipole-dipole interaction between Rydberg atoms"},"references":{"count":0,"internal_anchors":0,"resolved_work":0,"sample":[],"snapshot_sha256":"258153158e38e3291e3d48162225fcdb2d5a3ed65a07baac614ab91432fd4f57"},"source":{"id":"1705.03293","kind":"arxiv","version":1},"verdict":{"created_at":null,"id":null,"model_set":{},"one_line_summary":"","pipeline_version":null,"pith_extraction_headline":"","strongest_claim":"","weakest_assumption":""}},"verdict_id":null}}],"author_attestations":[],"timestamp_anchors":[],"storage_attestations":[],"citation_signatures":[],"replication_records":[],"corrections":[],"mirror_hints":[],"record_created":{"event_id":"sha256:5959ed205d0805d4fff84fb6b07dabeacef6658613a7491e36ba222dc245f46f","target":"record","created_at":"2026-05-18T00:38:41Z","signer":{"key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signer_id":"pith.science","signer_type":"pith_registry"},"payload":{"attestation_state":"computed","canonical_record":{"metadata":{"abstract_canon_sha256":"e524ce4d206fe76a773ade625406637962ab05a87440921468e336157f173cc4","cross_cats_sorted":["cond-mat.quant-gas","physics.atom-ph"],"license":"http://arxiv.org/licenses/nonexclusive-distrib/1.0/","primary_cat":"quant-ph","submitted_at":"2017-05-09T12:35:46Z","title_canon_sha256":"fff0d5bc5e233b186ca77360e8fc6c1d673d740900c074061a01978882de99bc"},"schema_version":"1.0","source":{"id":"1705.03293","kind":"arxiv","version":1}},"canonical_sha256":"9eebc0774fe7951fc88f81d5b5b173839f8465e52cb06cd9a59f4796bb08b6ab","receipt":{"algorithm":"ed25519","builder_version":"pith-number-builder-2026-05-17-v1","canonical_sha256":"9eebc0774fe7951fc88f81d5b5b173839f8465e52cb06cd9a59f4796bb08b6ab","first_computed_at":"2026-05-18T00:38:41.589762Z","key_id":"pith-v1-2026-05","kind":"pith_receipt","last_reissued_at":"2026-05-18T00:38:41.589762Z","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","receipt_version":"0.3","signature_b64":"C3Hmybogu0YUkRTqha4G0l0QUSN8ZMHBWbpQrT1j3v8/JBq8m+O/joskmvN2IeowtNiErITyyBCv9upqM0VlBw==","signature_status":"signed_v1","signed_at":"2026-05-18T00:38:41.590272Z","signed_message":"canonical_sha256_bytes"},"source_id":"1705.03293","source_kind":"arxiv","source_version":1}}},"equivocations":[],"invalid_events":[],"applied_event_ids":["sha256:5959ed205d0805d4fff84fb6b07dabeacef6658613a7491e36ba222dc245f46f","sha256:fe3b8130104326d282d91d304e1a20caf6dbb5805ced8ad65b7f2bc397b767e3"],"state_sha256":"3e4e6f1037f763aca3df075bdf0f317a640bb200e8bc12a0ba8242478268151e"},"bundle_signature":{"signature_status":"signed_v1","algorithm":"ed25519","key_id":"pith-v1-2026-05","public_key_fingerprint":"8d4b5ee74e4693bcd1df2446408b0d54","signature_b64":"kzsAMbwJo0fVNxUBJaRp86DCqeuJ4R346jef+gxM80EsogkJgsLAL0/RizL8zDcq0SrbT9Va8h/PlQkPYSwwBw==","signed_message":"bundle_sha256_bytes","signed_at":"2026-05-30T18:53:58.608684Z","bundle_sha256":"2b518d01750d20ed77d2bf2e416b464e1ce6fff51a343d4a266abad9ead621c7"}}